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31.
The randomly located trivalent silicon atoms are shown to account for the thermally generated interface states at the SiO2-Si interface. The interface state density is greatly reduced in water containing ambients at low temperatures (450°C) by forming trivalent silicon hydroxide bonds. Interface states are regenerated when the ?Si-OH bonds are broken by ionizing radiation and the OH ions are drifted away. In the bulk of the oxide film, the trivalent silicon and the interstitial oxygen donor centers are shown to be responsible for the heat and radiation generated positive space charge build-up (oxide charge) in thermally grown silicon oxide. 相似文献
32.
A ? network for carrier generation?recombination?trapping processes under arbitrary steady-state conditions is obtained, which has the following features which are useful for computer calculations of the admittance functions of semiconductor devices: the admittances are positive real, the voltage-controlled current sources are connected between the hole and electron quasi-Fermi potential nodes, and the current sources vanish at zero external excitation. 相似文献
33.
An exact 1-lump integral representation of a semiconductor layer of thickness w and its circuit model are obtained for large-signal and arbitrary steady-state levels. The dielectric capacitance is isolated from the distributed network. The application to p-n junctions is given as an illustration. 相似文献
34.
35.
This paper reports the DC steady-state current-voltage and conductance-voltage characteristics of a Bipolar Field-Effect Transistor(BiFET) under the unipolar(electron) current mode of operation,with bipolar(elec-tron and hole) charge distributions considered.The model BiFET example presented has two MOS-gates on the two surfaces of a thin pure silicon base layer with electron and hole contacts on both edges of the thin base.The hole contacts on both edges of the thin pure base layer are grounded to give zer... 相似文献
36.
This paper reports the physical realization of the Bipolar Field-Effect Transistor (BiFET) and its one-transistor basic building block circuits. Examples are given for the one and two MOS gates on thin and thick, pure and impure base, with electron and hole contacts, and the corresponding theoretical current-voltage characteristics previously computed by us, without generation-recombination-trapping-tunneling of electrons and holes. These ex-amples include the one-MOS-gate on semi-infinite thick impure base transistor (the bulk transistor) and the impure-thin-base Silicon-on-Insulator (SOI) transistor and the two-MOS-gates on thin base transistors (the FinFET and the Thin Film Transistor TFT). Figures are given with the cross-section views containing the electron and hole concen-tration and current density distributions and trajectories and the corresponding DC current-voltage characteristics. 相似文献
37.
本文报告了硅互补金属氧化层硅(CMOS)电压倒相电路的直流稳态电压和电流转移特性和功率耗散. 这电路用一只实际的﹑纳米尺度的双极场引晶体管(BiFET)实现. 通过数字求解五个偏微分方程,可获得这些电学特性. 方程是基于这种器件结构:在薄纯硅基层的两表面上各有一个MOS栅,在这薄基的两端都有电子和空穴接触. 内部条件和CMOS边界条件用于三种势(静电势和电子及空穴电化学势). 用一台装有Windows XP-PRO下的64位FORTRAN语言的双核个人计算机,快速地计算出一系列曲线. 相似文献
38.
场引晶体管本质双极,包括电子和空穴表面和体积沟道和电流,一或多个外加横向控制电场.自1952年Shockley发明,55年来它被认为单极场引晶体管,因电子电流理论用多余内部和边界条件,不可避免忽略空穴电流.多余条件,诸如电中性和常空穴电化电势,导致仅用电子电流算内部和终端电学特性的错误解.当忽略的空穴电流与电子电流可比,可在亚阈值区和强反型区,错误解有巨大误差.本文描述普适理论,含有电子和空穴沟道和电流.用z轴宽度方向均匀的直角平行六面体(x,y,z)晶体管,薄或厚、纯或杂基体,一或二块MOS栅极,描述两维效应及电势、电子空穴电化电势的正确内部和边界条件.没用多余条件,导出四种常用MOS晶体管,直流电流电压特性完备解析方程:半无限厚不纯基上一块栅极(传统的Bulk MOSFET),与体硅以氧化物绝缘的不纯硅薄层上一块栅极(SOI),在沉积到绝缘玻璃的不纯硅薄层上一块栅极(SOI TFT),和薄纯基上两块栅极(FinFETs). 相似文献
39.
本文描述半导体场引晶体管器件物理和理论所用的根本原则,它适用电场中有两种载流子的器件.讨论边界条件对器件电流电压特性的重要性.作为例子,计算两种边界条件下的转移直流电压特性:电势边界给出很高、流进内禀晶体管、飘移限制抛物型电流,电化学势边界仿真电子和空穴接触,给出很低、越过势垒注入、扩散限制电流,具有理想、每量级60mV、指数型亚阈值区倾斜.双MOS栅薄纯基硅场引晶体管为典型结构. 相似文献
40.
A multi‐frequency rectangular slot antenna for 4G‐LTE/WiMAX/WLAN and S/C/X‐bands applications is presented. The proposed antenna is comprised of rectangular slot, a pair of E‐shaped stubs, and an inverted T‐shaped stub and excited using staircase feed line. These employed structures help to achieve multiband resonance at four different frequency bands. The proposed multiband slot antenna is simulated, fabricated and tested experimentally. The experimental results show that the antenna resonates at 2.24, 4.2, 5.25, and 9.3 GHz with impedance bandwidth of 640 MHz (2.17‐2.82 GHz) covering WiMAX (802.16e), Space to Earth communications, 4G‐LTE, IEEE 802.11b/g WLAN systems defined for S‐band applications. Also the proposed antenna exhibits bandwidth of 280 MHz (4.1‐4.38 GHz) for Aeronautical and Radio navigation applications, 80 MHz (4.2‐4.28 GHz) for uncoordinated indoor systems,1060 MHz (5.04‐6.1 GHz) for the IEEE 802.11a WLAN system defined for C‐band applications and 2380 MHz (7.9‐10.28 GHz) defined for X‐band applications. Further, the radiation patterns for the designed antenna are measured in anechoic chamber and are found to agree well with simulated results. 相似文献